Year 11 PhysicsFundamentals of mechanics⏱ ~60 min5 MC · 3 Short AnswerLesson 27 of 28
Momentum and Impulse
Momentum, $p = mv$, measures how hard something is to stop, it combines mass and velocity into one quantity. Change it and you need an impulse: a force acting over a time, $Ft = \Delta p$. This single relationship explains why airbags save lives, why follow-through matters in sport, and why momentum is conserved whenever objects interact only with each other.
Today's hook: An airbag and a brick wall both stop you in a crash, but the airbag stops you over a longer time, which means a far smaller force. Same change in momentum, gentler force. The whole physics of crash safety is in the impulse equation $Ft = \Delta p$.
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Orient and predict
Before You Read
warm-up
A raw egg is dropped from the same height onto a concrete floor and onto a soft cushion. It breaks on the concrete but survives on the cushion.
Before reading: the egg's change in momentum is the same in both cases, so what is different that protects it on the cushion? Write your prediction and one sentence of reasoning.
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Intentions and key terms
Learning Intentions
goals
Know
That momentum is $p = mv$, a vector quantity
That impulse $= Ft = \Delta p$, the change in momentum
The condition for momentum conservation: no external net force
Understand
Why a longer impact time means a smaller force
Why momentum is conserved in collisions (Newton's third law)
That impulse is the area under a force–time graph
Can Do
Calculate momentum with $p = mv$
Apply $Ft = \Delta p$ to find a force or time
Explain a safety device using impulse
Scan these before reading
vocab
Momentum ($p$)The product of mass and velocity, $p = mv$; a vector measured in $\text{kg m s}^{-1}$.
ImpulseThe change in momentum produced by a force acting over a time: impulse $= Ft = \Delta p$, in $\text{N s}$.
Isolated systemA system with no net external force; its total momentum stays constant.
Conservation of momentumIn an isolated system, total momentum before equals total momentum after.
Where this sits in the course: Momentum is the second great conserved quantity of mechanics, alongside energy (L24–L26). The impulse relation $Ft = \Delta p$ is really Newton's second law in disguise. This sets up the collision analysis and practical in Lesson 28, the final lesson of the focus area.
Misconceptions To Fix
watch out
✗ Wrong: A cushion reduces the change in momentum when stopping an object.
✓ Right: The change in momentum is the same; the cushion increases the time, which reduces the force ($F = \Delta p / t$).
✗ Wrong: Momentum and kinetic energy are the same thing.
✓ Right: Momentum is $p = mv$ (a vector); kinetic energy is $\tfrac{1}{2}mv^2$ (a scalar). They behave differently in collisions.
Core Content
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Momentum: Mass in Motion
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Momentum: Mass in Motion
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How hard something is to stop, $p = mv$
Momentum captures how much "oomph" a moving object has, combining how heavy it is with how fast it moves, and that is what makes it hard to stop.
Momentum is the product of an object's mass and velocity, given on the NESA formula sheet by:
$$p = mv$$
It is a vector, pointing in the same direction as the velocity, measured in $\text{kg m s}^{-1}$. A heavy slow truck and a light fast bullet can have similar momentum. Because momentum is a vector, direction matters, a $5\ \text{kg m s}^{-1}$ momentum to the right is different from one to the left, which becomes vital in collisions.
Momentum is $p = mv$, a vector in the direction of the velocity, measured in $\text{kg m s}^{-1}$. It combines mass and speed into a single measure of how hard an object is to stop; direction matters because momentum is a vector.
Pause, copy the highlighted definition into your book before moving on.
Did you get this? A $1200\ \text{kg}$ car travels at $15\ \text{m s}^{-1}$. Its momentum is…
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Impulse: Changing Momentum, $Ft = \Delta p$
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Impulse: Changing Momentum, $Ft = \Delta p$
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A force acting over time changes momentum, and longer times mean gentler forces
We just defined momentum as $p = mv$. That raises a question: what does it take to change an object's momentum? This card answers it → an impulse, a force applied over a time, equal to the change in momentum: $Ft = \Delta p$.
To change momentum you must apply a force for a length of time, and the same momentum change can come from a big force briefly or a small force for longer.
Impulse is the change in momentum, produced by a force acting over a time interval. On the NESA formula sheet:
$$\text{impulse} = Ft = \Delta p = mv - mu$$
Rearranging gives $F = \dfrac{\Delta p}{t}$: for a fixed change in momentum, a longer impact time $t$ means a smaller force $F$. This is exactly why airbags, crumple zones, and bending your knees when landing all reduce injury, they extend the stopping time.
WORKED EXAMPLE · IMPULSE AND FORCE
A $0.15\ \text{kg}$ cricket ball travelling at $30\ \text{m s}^{-1}$ is caught and brought to rest. Compare the average force if it is stopped in $0.020\ \text{s}$ (rigid hands) versus $0.10\ \text{s}$ (giving with the catch).
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GIVEN: $m = 0.15\ \text{kg}$, $u = 30\ \text{m s}^{-1}$, $v = 0$; $t_1 = 0.020\ \text{s}$, $t_2 = 0.10\ \text{s}$. FIND: average force in each case.
The change in momentum is the same; only the time differs.
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METHOD: $$\Delta p = m(v - u) = 0.15(0 - 30) = -4.5\ \text{kg m s}^{-1}$$ then $$F = \frac{\Delta p}{t}$$
The magnitude of $\Delta p$ is $4.5\ \text{kg m s}^{-1}$; use it with each time.
Check: a 5× longer stopping time gives a 5× smaller force, softer catch, gentler force. ✓
The cricket-ball worked example, as average forces. Both rectangles have the same area, so both catches give the same change in momentum.Text description
Force axis in newtons; time axis 0 to 0.10 s.
Rigid hands: an average force F₁ for 0.020 s (tall, narrow rectangle).
Giving with the catch: an average force F₂ for 0.10 s (low, wide rectangle), five times as long.
Each area is the impulse, F × t, equal to the ball's change in momentum, so the two areas are equal. The worked example finds F₁ and F₂.
Impulse equals the change in momentum: $Ft = \Delta p = mv - mu$. Since $F = \Delta p / t$, a longer impact time gives a smaller force. Catching the ball in $0.020\ \text{s}$ needs $225\ \text{N}$, but giving with it over $0.10\ \text{s}$ needs only $45\ \text{N}$.
Add the highlighted relationship to your notes before the check below.
Quick check: The same change in momentum is delivered over twice the time. The average force is…
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Apply it yourself
Activity 1
ApplyBand 5
Impulse and Safety
Pattern B, Calculate then explain
A $70\ \text{kg}$ person moving at $8.0\ \text{m s}^{-1}$ is brought to rest in a collision. In your book: (1) calculate their change in momentum; (2) calculate the average force if stopped in $0.10\ \text{s}$ (no airbag) and in $0.50\ \text{s}$ (with airbag); (3) write two sentences explaining, in terms of $Ft = \Delta p$, how an airbag reduces the force on the person and therefore the risk of injury.
Odd one out: three of these are ways to reduce the force in a collision for a given change in momentum. Which one is not?
Dot point: Solve problems involving momentum using p = mv and impulse = Ft = Δp
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Why Momentum Is Conserved in Collisions
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Why Momentum Is Conserved in Collisions
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Newton's third law guarantees the total momentum is unchanged
We just used impulse to change one object's momentum. That raises a question: when two objects collide, why does their total momentum stay the same? This card answers it → because they push on each other with equal and opposite forces for the same time (Newton's third law).
In a collision, the two objects push on each other equally and oppositely, so whatever momentum one gains, the other loses, the total is unchanged.
The condition for momentum conservation is that the system is isolated, no net external force acts on it. During a collision, the two objects exert equal and opposite forces on each other (Newton's third law) for exactly the same contact time. So the impulse on object A is equal and opposite to the impulse on object B: $F t$ on one equals $-F t$ on the other. Therefore the momentum gained by one is exactly the momentum lost by the other, and the total momentum is unchanged:
This holds for any collision, whether the objects bounce apart or stick together, as long as no outside force interferes.
Momentum is conserved when no net external force acts (an isolated system). In a collision the objects exert equal and opposite forces for the same time (Newton's third law), so the impulses are equal and opposite, one gains exactly the momentum the other loses. Thus $\sum p_{before} = \sum p_{after}$.
Pause, copy the highlighted reasoning into your book before the check below.
Last check: Decide if the statement is true or false.
Total momentum is conserved in a collision because the colliding objects exert equal and opposite forces on each other for the same time.
Match each statement about momentum with whether it is a condition, a definition or a consequence:
$p = mv$
The system must be isolated, with no net external force
The forces in a collision are equal and opposite for the same time
$\text{impulse} = Ft = \Delta p$
The condition for momentum conservation
The impulse-momentum relationship
The definition of momentum
The third-law reason momentum is conserved
Dot point: State the conditions under which momentum is conserved
✓
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Show what you have learned
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Multiple Choice
+5 XP
A fresh set drawn from this lesson's question bank, feedback shown immediately. +5 XP per correct · +25 XP all correct
Pick your answer, then rate your confidence, that tells the system what to drill next.
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Short Answer
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UnderstandBand 5(4 marks) 1. Using the concept of impulse, explain why a car's crumple zone reduces the force on the occupants during a crash. Refer to the relationship $Ft = \Delta p$.
1 mark: states impulse $Ft = \Delta p$ · 1 mark: the change in momentum is fixed by the crash · 1 mark: the crumple zone increases the collision time $t$ · 1 mark: since $F = \Delta p / t$, a larger $t$ gives a smaller force, reducing injury
ApplyBand 5(4 marks) 2. A $0.15\ \text{kg}$ cricket ball travelling at $30\ \text{m s}^{-1}$ is caught and brought to rest in $0.40\ \text{s}$. Calculate the change in momentum and the average force on the ball, and explain why a fielder pulls their hands back.
1 mark: $\Delta p = 4.5\ \text{kg m s}^{-1}$ · 1 mark: applies $Ft = \Delta p$ · 1 mark: $F = 11.25\ \text{N}$ · 1 mark: pulling back increases $t$, and since $\Delta p$ is fixed, $F$ falls
Dot point: Solve problems involving momentum using p = mv and impulse = Ft = Δp
UnderstandBand 6(3 marks) 3. Explain, using Newton’s third law, why the total momentum of two colliding objects is conserved, and state the condition that must hold.
1 mark: the two forces are equal in magnitude and opposite in direction · 1 mark: they act for the same time, so the impulses are equal and opposite · 1 mark: the momentum changes cancel, provided the system is isolated from net external forces
Dot point: Explain why momentum is conserved during collisions
Show all answers
Multiple choice
MC answers and full explanations are shown inline as you complete each question. Use the retry button to attempt a fresh set from the lesson bank.
Short Answer Model Answer
Q1 (4 marks): Impulse is the change in momentum, $Ft = \Delta p$. In a crash the occupant's change in momentum is fixed, they must go from their travelling speed to rest. A crumple zone deforms on impact, extending the time $t$ over which this momentum change occurs. Since $F = \dfrac{\Delta p}{t}$, increasing the collision time $t$ for the same $\Delta p$ reduces the average force $F$ acting on the occupants. The smaller force means a lower risk of injury, which is the purpose of the crumple zone.
Q2 (4 marks): Taking the initial direction as positive, the momentum changes from $p_i = 0.15 \times 30 = 4.5\ \text{kg m s}^{-1}$ to zero, so $$\Delta p = 0 - 4.5 = -4.5\ \text{kg m s}^{-1}$$ a magnitude of $4.5\ \text{kg m s}^{-1}$ directed against the original motion. From the impulse-momentum relationship $Ft = \Delta p$, $$F = \frac{\Delta p}{t} = \frac{4.5}{0.40} = 11.25\ \text{N}$$ A fielder pulls their hands back because the change in momentum is fixed by the ball’s mass and speed and cannot be altered. Only the time is under the fielder’s control, and since $F = \Delta p / t$, lengthening the stopping time reduces the average force proportionally. Doubling the time halves the force on both the ball and the hands.
Q3 (3 marks): During the collision each object exerts a force on the other. By Newton’s third law those two forces are equal in magnitude and opposite in direction, and they necessarily act for exactly the same duration, since the contact begins and ends at the same instants for both. The impulse each object receives is $Ft$, so the two impulses are also equal in magnitude and opposite in direction. Since impulse equals change in momentum, the momentum gained by one object is exactly the momentum lost by the other, and the total momentum of the pair is unchanged. The condition is that the system is isolated: no net external force acts on it during the collision, or the collision is brief enough that any external impulse is negligible compared with the internal one.
✓
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Retrieve, reflect and finish
Lock it in
boss
You can now calculate momentum with $p = mv$, apply impulse $Ft = \Delta p$, and explain why momentum is conserved in collisions. The final lesson uses this to analyse elastic and inelastic collisions in a practical.
At the start you predicted what protects the egg on the cushion. The answer: the change in momentum is the same, but the cushion increases the time of impact, so by $F = \Delta p / t$ the force on the egg is much smaller, small enough not to break it. If you thought the cushion changed the momentum, revisit Card 2.
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Check what actually stuck
A short spaced-retrieval set, mixing this lesson with earlier ones. It gets harder to guess and easier to remember.